Optical interleaver and filter cell design with enhanced thermal stability

ABSTRACT

An optical interleaver for use in a range of telecommunications applications including optical multiplexers/demultiplexers and optical routers. The optical device includes an optical processing loop which allows multi-stage performance characteristics to be achieved with a single physical filtration stage. Optical processing on the first leg and second legs of the loop is asymmetrical thereby improving the integrity of the optical signals by effecting complementary chromatic dispersion on the first and second legs. A fundamental filter cell within the interleaver filters optical signals propagating on each of the two legs of the optical loop which intersects the fundamental filter cell.

CROSS-REFERENCE TO RELATED APPLICATIONS

[0001] This application is a continuation-in-part of application Ser.No. 10/170,055 entitled “METHOD AND APPARATUS FOR AN OPTICAL MULTIPLEXERAND DEMULTIPLEXER WITH AN OPTICAL PROCESSING LOOP” filed Jun. 12, 2002,which is incorporated by reference in its entirety.

BACKGROUND OF THE INVENTION

[0002] 1. The Field of the Invention

[0003] The present disclosure generally relates to optical interleavers,filters, and components, and more particularly to optical interleavers,filters, and components for optical fiber communication networks.

[0004] 2. Background and Related Art

[0005] The Synchronous Optical Network (SONET) standard defines ahierarchy of multiplexing levels and standard protocols which allowefficient use of the wide bandwidth of fiber optic cable, whileproviding a means to merge lower level DS0 and DS1 signals into a commonmedium. Currently optical communication is accomplished by what is knownas “wavelength division multiplexing” (WDM), in which separatesubscriber/data sessions may be handled concurrently on a single opticfiber by means of modulation of each of those subscriber data streams ondifferent portions, a.k.a. channels, of the light spectrum.

[0006] The spacing between channels is constantly being reduced as theresolution and signal separation capabilities of multiplexers anddemultiplexers are improved. Current International TelecommunicationsUnion (ITU) specifications call for channel separations of approximately0.4 nm, i.e., 50 GHz. At this channel separation as many as 128 channelsmay be supported in C-band alone. Each channel is modulated on aspecific center frequency, within the range of 1525-1575 nm, with thecenter frequency of each channel provided by a corresponding one of 128semiconductor lasers. The modulated information from each of thesemiconductor lasers is combined (multiplexed) onto a single optic fiberfor transmission. As the length of a fiber increases the signal strengthdecreases. To offset signal attenuation erbium doped fiber amplifiers(EDFAs) are used at selected locations along the communication path toboost signal strength for all the channels. At the receiving end theprocesses is reversed, with all the channels on a single fiber separated(demultiplexed), and demodulated optically and/or electrically.

[0007] Optical filters play important roles in handling these opticalcommunications for the telecommunications industry. They performwavelength multiplexing and demultiplexing of the 128 or more opticalchannels. They may also be used to gain scale EDFAs by flattening theirgain profile.

[0008] The requirements for optical filters used for any of theseapplications are very demanding. The close spacing between the channelsin a WDM, makes it desirable to design a WDM with flat pass bands inorder to increase the error tolerance. This is primarily because thecenter wavelength of a transmitter slips with temperature. Further, thecascading of the WDM stages causes the pass bands to become narrower ateach WDM down the chain. Therefore, the larger the pass bands thegreater the shift tolerance of the channel. With faster data rates, itis also becoming increasingly important to reduce or eliminate sourcesof chromatic dispersion while processing optical signals.

[0009] Optical filters also experience problems with respect to thermalstability. Like transmitters, the performance characteristics of opticalfilters change with temperature. As indicated above, however, therequirements for optical filters are quite demanding and seem to be everincreasing. While it is possible to actively compensate for poor thermalstability in order to meet specified performance characteristics, activecompensation can add significant complexity and cost to filter designs.

[0010] Various devices, such as multi-stage band and comb splitters,have been proposed to fill these new demanding requirements and none arefully satisfactory. In a multi-stage band splitter, the first stagemakes a coarse split of two wavelength ranges, and subsequent stagesmake finer and finer splits of sub-bands within each of the wavelengthranges. In a multi-stage comb splitter, the first demultiplexing stagefilters out two interlaced periodic sets of relatively narrow bandpasses and the subsequent stages employ wider band pass periodic filtersuntil the individual channels are demultiplexed. In either case, noiseand inter-channel interference are limiting factors in the handling ofincreasingly narrow band pass requirements. Multi-layer thin-filmfilters can be used to construct optical filters in bulk optics, butthey are undesirable because of an increase in the number of layers fornarrow channel spacing, precision of manufacture and expense associatedwith increasingly narrow band pass requirements. Further, dispersionwill become a major issue as channel spacing decreases. Especially at 50GHz channel spacing, dispersion of thin film filters is so big that itcan not be used for an OC-192 signal (10 Gbit/sec). Mach-Zehnderinterferometers have been widely employed, but they have a sinusoidalresponse giving rise to strongly wavelength dependent transmission and anarrow rejection band. Other designs have encountered a variety ofpractical problems.

[0011] Accordingly, there is a need for new optical filters andcomponents with enhanced thermal stability for a variety of opticalapplications

BRIEF SUMMARY OF THE INVENTION

[0012] In general, an optical interleaver, filter cell, and componentdesign is provided for use in a wide range of telecommunications,network, and other applications, generally including opticalmultiplexers/demultiplexers and optical routers. In one exampleembodiment, an optical interleaver splits and combines optical signalsof frequency division multiplexed optical communication channels whichare evenly spaced apart in frequency from one another. The opticalinterleaver includes an optical processing loop which allows multi-stageperformance characteristics to be achieved with a single physicalfiltration stage. Optical processing on the first leg and second legs ofthe loop improves the integrity of the optical signals by effectingcomplementary chromatic dispersion on the first and second processinglegs. The single physical filtration stage includes a fundamental filtercell and may include one or more harmonic filters. Waveplates may beused to rotate polarization in order to adjust splitting ratios and inorder to align interleaver components for more convenient packaging.

[0013] In another example embodiment, the optical interleaver forprocessing optical signals includes a fundamental filter cell, a retroreflector and an optical polarization beam displacer. The fundamentalfilter cell filters optical signals propagating on each of two legs ofan optical loop which intersects the fundamental filter cell. Thefundamental filter cell operates as a full waveplate to one set of oneor more optical signals and a half waveplate to another set of one ormore optical signals on a selected one of the two legs and as a halfwaveplate to the one set of one or more optical signals and a fullwaveplate to the other set of one or more optical signals on a remainingone of the two legs. The retro reflector optically couples with thefundamental filter cell to reflect the optical signals from one of thetwo legs to the other of the two legs to form the optical loop. Theoptical polarization beam displacer optically couples between thefundamental filter cell and the retro reflector to split or combine theoptical signals depending on the polarization and propagation directionof the optical signals along the optical loop. Based on the particularimplementation, the sets of one or more optical signals may correspondto an odd set of channels and an even set of channels, or may correspondto one or more arbitrary optical signals that are interleaved or are tobe interleaved with one or more other optical signals, and so forth.

[0014] In an alternate embodiment of the invention, an opticalinterleaver for processing optical signals between a first portcommunicating one set of one or more optical signals together withanother set of one or more optical signals and second and third portsseparately communicating the sets of optical signals is disclosed. Theoptical interleaver includes: a fundamental filter cell, a retroreflector, and an optical polarization beam displacer. The fundamentalfilter cell optically couples on one side to all of the ports.

[0015] The fundamental filter cell exhibits a first and a second freespectral range (FSR) to optical signals propagating on an optical loopwith a first leg coupled to the first port and a second leg coupled tothe second and third ports. The first and second FSRs are offset withrespect to one another to effect substantially complementary chromaticdispersions for each optical signal. The retro reflector opticallycouples with the fundamental filter cell to reflect the optical signalsfrom one of the legs to the other of the legs to form the optical loop.The optical polarization beam displacer optically couples between thefundamental filter cell and the retro reflector to split or combine theoptical signals depending on the polarization and propagation directionof the optical signals along the optical loop.

[0016] In some embodiments, a polarization beam splitting cell (e.g.,that may be used within a filter cell) is mounted horizontally toimprove the filter cell's thermal stability.

[0017] Additional features and advantages of the invention will be setforth in the description which follows, and in part will be obvious orapparent from the following detailed description and accompanyingdrawings, or may be learned by practicing of the invention. The|features and advantages of the invention may be realized and obtainedby means of the instruments and combinations particularly pointed out inthe appended claims. These and other features of the present inventionwill become more fully apparent from the following description andappended claims, or may be learned by practicing of the invention as setforth hereinafter.

BRIEF DESCRIPTION OF THE DRAWINGS

[0018] In order to describe the manner in which the above-recited andother advantages and features of the invention can be obtained, a moreparticular description of the invention briefly described above will berendered by reference to specific embodiments thereof which areillustrated in the appended drawings. Understanding that these drawingsdepict only typical embodiments of the invention and are not thereforeto be considered as limiting its scope, the invention will be describedand explained with additional specificity and detail through the use ofthe accompanying drawings in which:

[0019]FIG. 1 is a hardware block diagram of an embodiment of an opticalinterleaver with an optical processing loop formed by a single physicalstage coupled to an optical polarization beam displacer and retroreflector.

[0020] FIGS. 2A-B are isometric views of alternate embodiments of theoptical interleaver shown in FIG. 1 with birefringent crystals formingthe single physical filter stage.

[0021] FIGS. 3A-B are isometric views of alternate embodiments of theoptical interleaver shown in FIG. 2 with optical filter cells formingthe single physical filter stage.

[0022]FIG. 4A and FIG. 4C are top and side hardware block views of theembodiment of the optical interleaver shown in FIG. 3A.

[0023]FIG. 4B is a polarization diagram showing polarization vectorsalong the two legs of the optical processing loop formed within theembodiment of the optical interleaver shown in FIG. 3A.

[0024]FIG. 5A is an isometric view of a polarization beam splitting cellutilized in the embodiment of the optical interleaver shown in FIGS.3A-B with polarization dependent beam splitters linked by a pair ofdelay paths.

[0025]FIG. 5B shows the fast and slow delay paths within the cell shownin FIG. 5A.

[0026]FIG. 5C is an isometric view of a linearly polarized opticalsignal in relation to the polarization axis of the polarization beamsplitting cell shown in FIG. 5A.

[0027] FIGS. 5D-E show polarization diagrams for opposing sides of thepolarization beam splitting cell shown in FIG. 5A.

[0028]FIG. 5F shows an isometric view of an example polarization beamsplitting cell mounted vertically on a base.

[0029]FIG. 5G shows an isometric view of an example polarization beamsplitting cell mounted horizontally on a base.

[0030]FIG. 5H is a graph comparing wavelength angle sensitivity for theexample polarization beam splitting cells mounted vertically in FIG. 5Fand horizontally in FIG. 5G.

[0031]FIG. 6A is an isometric view of a multi-cell implementation of thepolarization beam splitting cell shown in FIG. 5A utilized in theembodiment of the optical interleaver shown in FIG. 3A.

[0032] FIGS. 6B-C show polarization diagrams for opposing ends of thepolarization beam splitting cells shown in FIG. 6A.

[0033]FIG. 6D is a side elevation view of the delay paths of themulti-cell implementation shown in FIG. 6A.

[0034]FIG. 6E is a side elevation view of the variable coupling betweencells of the multi-cell implementation shown in FIG. 6A.

[0035]FIG. 6F shows the individual transforms associated with each ofthe four delay paths on one of the two optical processing legs throughthe two cell sequence shown in FIG. 6A.

[0036]FIG. 7A-B are graphs showing the complementary dispersionsprofiles about a representative center frequency of one of the channels.

[0037]FIG. 8A-E are signal diagrams showing filter functions at variouslocations along the optical path of the interleaver shown in FIG. 1.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0038] Various optical interleavers, filter cells, and opticalcomponents are disclosed that can be used in a range oftelecommunications an other applications including opticalmultiplexers/demultiplexers and optical routers. An example opticalinterleaver embodiment includes an optical processing loop which allowsmulti-stage performance characteristics to be achieved with a singlephysical filtration stage. Optical processing on the first leg andsecond leg of the loop improves the integrity of the optical signals byeffecting complementary chromatic dispersion on the first and secondlegs.

[0039]FIG. 1 is a hardware block diagram of an embodiment of an opticalinterleaver 100 with an optical processing loop 130, 162, 132 formed bya single stage 104 optically coupled to a splitter/combiner 150 andretro reflector 160. As used in this application, optically coupledshould be interpreted broadly to encompass optical signal passingbetween two optical components directly, without any intervening opticalcomponents, as well as optical signals passing between two opticalcomponents using or through one or more intervening optical components.The interleaver is designed to operate on the narrowly spaced frequencydivision multiplexed channels of a telecommunications grid. Thesechannels may be spaced apart in frequency at 50 GHz intervals or less.The interleaver can, depending on the propagation direction of anoptical signal, split or combine an optical stream with 50 GHz channelspacing into two separate optical streams with odd and even 100 GHzchannel spacing respectively and vice versa. The interleaverseparates/combines optical signals, such as odd and even channel sets,with a higher degree of isolation and a lower dispersion than prior artdesigns. It may be used alone or in combination with other stages ofsimilar or different design to separate out and/or route opticalsignals, such as each individual channel of a telecommunications orother communication grid. Although embodiments of the invention aredescribed below in connection with odd and even channels sets forclarity, it should be appreciated that in general, embodiments of theinvention may process arbitrary sets of one or more optical signalswithin a stream of (or interleaved with) one or more other opticalsignals.

[0040] In operation, as an optical demultiplexer for example, opticalsignals with both odd channels and even channels are injected into port102 and are subject in stage 104 to a first stage of optical processingin leg 130 of the optical processing loop. The processed optical signalsfrom leg 130 are split in splitter 150 into discrete optical signalswith a corresponding one of an odd set of channels and an even set ofchannels and reflected by retro reflector 160 back to stage 104 for asecond stage of optical processing in leg 132 of the optical processingloop. The resultant optical signals, one with odd channels and the otherwith the even channels, are output at the corresponding one of port 188,198. Where the operations are reversed the optical interleaver 100operates as an optical multiplexer combining discrete optical signals,one with odd channels and the other with even channels, input at ports188, 198 into a single optical signal with both odd and even channelsoutput at port 102.

[0041] Stage 104 includes a fundamental filter cell 120 and may includeadditional harmonic filters 140, 144. The filters are, in one embodimentof the invention, polarization filters which accept polarized opticalsignals and which split the input into orthogonal component vectorsalong a fast and a slow delay path. The optical pathlength differencebetween the fast and slow delay paths determines the periodic combfilter functions exhibited by the fundamental filter cell. The filtersmay be fabricated from a range of birefringent materials (see FIGS.2A-B) or from the elements of a polarization beam splitting cell (seeFIGS. 3A-B). The filters of stage 104 may be characterized with aFourier series in which the fundamental filter cell provides fundamentalcomb filter functions and in which any additional harmonic filtersimpose higher order harmonics thereon.

[0042] The fundamental filter cell is designed with a first freespectral range (FSR) for optical signals propagating on the first leg130 and a second FSR for optical signals propagating on the second leg132 of the optical processing loop. The first and the second FSR areboth substantially equal to the channel spacing between adjacent odd oreven channels. The first and second FSR are also offset with respect toone another by an amount which effects phase shifts of odd integermultiples of substantially half a wavelength for each center wavelengthassociated with any of the channels, odd or even. This asymmetryimproves the integrity of the optical signals by effecting complementarychromatic dispersion on the first and second legs.

[0043] The offset in FSR between the first and second legs of opticalprocessing in the fundamental filter cell 120 is effected in theembodiment shown in FIG. 1 by a fundamental filter 122 optically coupledon one of the optical processing legs 126 128 with a zero-order halfwaveplate 124. In this embodiment of the invention the fundamentalfilter operates as a narrowband waveplate with an FSR on each of thelegs which substantially corresponds with the spacing between adjacentodd or even channels. In this embodiment the fundamental filter operatesas a narrowband full/half waveplate or half/full waveplate for the oddset of channels and the even set of channels. The zero-order halfwaveplate may be a discrete component or integrated with the fundamentalfilter. As a discrete component the zero-order half waveplate may beoptically coupled with the fundamental filter on either side thereof.The zero-order half waveplate optically couples to the fundamentalfilter on one of the two legs of the optical loop. The zero-order halfwaveplate exhibits a second FSR which effects phase retardations of oddinteger multiples of substantially half a wavelength for each centerwavelength associated with the channels, odd or even.

[0044] The first and the second FSR of the fundamental filter cell eachsubstantially corresponds with the periodic frequency spacing betweenadjacent odd or even channels, e. g. an odd channel and an adjacent oddchannel. The optical path length difference between the two delay pathsin the fundamental filter cell on either the first or the second leg,corresponds inversely with the free spectral range (FSR). Thisrelationship is set forth in the following Equation 1: $\begin{matrix}{{FSR} = ( \frac{c}{{L_{S} - L_{F}}} )} & {{Equation}\quad 1}\end{matrix}$

[0045] where L_(S) and L_(F) are the total optical path length of eachof the delay paths on either of the optical processing legs within thefundamental filter cell and c is the speed of light in a vacuum.Additional filters, e. g. 140, 144 may provide the harmonics requiredfor establishing a flat top composite comb filter function for theinterleaver such as that shown in FIG. 8E. The interleaver showsimprovements in chromatic dispersion over prior art designs as a resultof an optical pathlength shift and inversely corresponding FSR offset onthe first and second optical processing leg within the fundamentalfilter cell 120.

[0046] In the embodiment of the invention shown in FIG. 1, thefundamental filter cell includes the zero-order half waveplate filterportion 124 on one of the optical processing legs 130, 132. Thiszero-order half waveplate filter imposes a half wavelength phaseretardation on both the odd and even channels. This zero-order halfwaveplate portion effects an optical pathlength difference in one of theoptical processing legs with respect to the other within the fundamentalfilter cell. The optical pathlength difference corresponds with oddinteger multiples of one-half of the wavelength of interest as shown inthe following Equation 2: $\begin{matrix}{{{OPD}_{L1} + {( {{2N} + 1} )( \frac{\lambda}{2} )}} = {OPD}_{L2}} & {{Equation}\quad 2}\end{matrix}$

[0047] where OPD_(L1) is the optical pathlength difference of thefundamental cell along one of the optical processing legs 130, 132 andOPD_(L2) is the optical pathlength difference of the fundamental cellalong the other of the optical processing legs 130, 132. This shift inoptical pathlength difference and inversely corresponding offset in FSRon the two optical processing legs 103, 132 results in substantiallycomplementary chromatic dispersion profiles along each of the opticalprocessing legs, the net effect of which is a substantial reduction ofchromatic dispersion and a concomitant improvement in signal integritywithin each telecommunications channel as shown in FIGS. 7A-B. Thisshift is achieved with a negligible deviation, e. g. less than 0.3%,between the first and second FSR of the fundamental cell 110.

[0048] The FSR of the zero-order half waveplate is expressed in thefollowing Equation 3: $\begin{matrix}{{FSR} = {( \frac{c}{{L_{S} - L_{F}}} ) = \frac{v_{c}}{{1/2} + m}}} & {{Equation}\quad 3}\end{matrix}$

[0049] where L_(S) and L_(F) are the total optical path length on thefast and slow delay paths of the zero-order half waveplate, ν_(c) is thecenter frequency of a selected one of the odd or even channels and m isthe integer order of the wavelength. The range of acceptable values forthe order m depends on the number of channels, the overall bandwidth,and the center frequency of the center channel. Smaller values of orderm correspond with more uniform the behavior of the zero-order halfwaveplate across all channels and smaller optical pathlengths. For atypical telecommunication application order m will be less thanone-hundred and may be in the range of 1-10. For a channel spacing of 50GHz the FSR of the zero-order half waveplate at a center frequency of1550 nm and an order of “0” would be 2*c[nm]/1550[nm] or approximately386 THz which is at least two orders of magnitude greater then the FSRof the fundamental filter 122.

[0050] FIGS. 2A-B are isometric views of alternate embodiments of theoptical interleaver shown in FIG. 1 with birefringent crystals formingthe fundamental and harmonic filters of the single filter stage. Theinterleaver 200 has 3 ports 102, 188, 198 which couple with thefundamental filter cell 220 via corresponding port couplers 210, 282,292 respectively. The port coupler 210 for port 102 includes: acollimator 212 with a lens, a beam splitter 214, and waveplates 216. Inoperation as an optical demultiplexer, an optical signal with odd andeven channels modulated thereon enters collimator 212 via port 102 whichmay be an optical fiber. The lens for collimator 212 may be a GradedIndex of Refraction (GRIN) or other lens system. The lensfocuses/collimates light depending on the propagation direction to/fromthe beam splitter 214. The beam splitter may be fabricated from abirefringent crystal with an optic axis oriented to effect a walk-off ofthe optical signal onto waveplates 216. The waveplates are zero-orderwaveplates and have optical axis oriented to effect a linearization ofthe polarization vectors of the two rays formed by the beam splitter.

[0051] The linearly polarized rays are then introduced into thefundamental filter cell 220, which includes a fundamental filter 222 anda zero-order half waveplate 124. The fundamental filter operates as anarrowband full and half or half and full waveplate for the odd and evenchannels respectively. The angle of the polarization vector for thelinearly polarized rays with respect to the optical axis 226 of thefundamental filter cell determines the coupling of the optical signalonto the fast and slow paths, e. g. the “e” and “o” rays in thefundamental filter. The harmonic filter cell 240 optically couples withthe fundamental filter cell and imposes a higher order harmonic on theoptical signals processed in the fundamental filter. The angle of thepolarization vector for the linearly polarized rays from the fundamentalcell with respect to the optical axis 242 of the harmonic filter celldetermines the coupling of the optical signal onto the fast and slowpaths, e. g. the extraordinary “e” and ordinary “o” rays in the harmonicfilter cell.

[0052] The optical polarization beam splitter/combiner/displacer 250splits the odd and even signal outputs on the first optical processingleg from the fundamental filter cell and the harmonic filter cell. Theretro reflector 160 then couples these split optical signals back intothe first stage, i.e. the harmonic filter cell 240 and the fundamentalfilter cell where they will be further isolated. The zero-order halfwaveplate 124 is optically coupled to the fundamental filter 222 on oneof the optical processing legs to effect a substantial reduction ofchromatic dispersion of the demultiplexed odd and even channels. Thefundamental filter beam benders 272, 280, 290 direct optical signalswith odd channels and optical signals with even channels to acorresponding one of the two output ports 188, 198 of the demultiplexervia an associated one of the port couplers 282, 292. In operation as amultiplexer the propagation path between the ports 198, 188 and port 102is reversed.

[0053] In the above embodiment illustrated in FIG. 2A, the optical axis226 of the fundamental cell and optical axis 242 of the harmonic cellare oriented perpendicular to each respective cell top surface. To forman angle between the polarization direction of the incident light andthe optical axis to effect polarization beam splitting, the fundamentalcell or the harmonic cell may be physically rotated with respect to thesignal propagation direction as indicated in FIG. 2A, especially in thecase which the polarization direction of incident light is vertically orhorizontally polarized. In some cases, for ease of packaging andmanufacturing, it is desirable to have the fundamental cell and theharmonic cell sit flat on a packaging platform. In such a case, thebirefringent crystals in the fundamental cell or the harmonic cells canbe cut in such a way that their respective optical axes 226 and 242 areoriented in predetermined angles with respect to the direction of theirrespective top surfaces, resulting in effective polarization beamsplitting. Thus, physical rotations of the fundamental or harmonic cellsare not required. Alternatively, if the optical axes of 226 and 242remain orientated perpendicular to their respective cell top surfaces,zero-order waveplates can be inserted in front of the fundamental celland the harmonic cell, leading to effective polarization beam splittingas explained below in connection with FIG. 2B.

[0054]FIG. 2B shows an alternate embodiment of the optical interleavershown in FIG. 2A. In FIG. 2B the optical interleaver 202 includeszero-order waveplates 270, 232 which allow alignment of externalfeatures of the fundamental filter 222, the zero-order half waveplate124 and the harmonic filter cell 240. Zero-order waveplate 270 allowsexternal features, e. g. surfaces of the fundamental filter 222 and thezero-order half waveplate 124 to be aligned with the port couplers 210,282, 292 via rotation of the optical signals entering and exiting thefundamental filter without effecting of the coupling ratio at whichoptical signals couple onto the fast and slow paths within thefundamental filter. Zero-order waveplate 232 allows external featurese.g. surfaces of the harmonic filter 240 to be aligned with thefundamental filter 222 and the zero-order half waveplate 124 withouteffecting of the coupling ratio at which optical signals couple to/fromthe fast and slow paths of the fundamental filter and the harmonicfilter.

[0055] FIGS. 3A-B are isometric views of alternate embodiments 300 and302 of the optical interleaver shown in FIGS. 2A-B with polarizationbeam splitting cells 322 and 340 and zero-order half waveplate 124forming the single filter stage. These cells will be discussed ingreater detail in the following FIGS. 4-6. In the embodiment shown inFIG. 3B external features of the polarization beam splitting cells 322,340 and the zero-order half waveplate 124 may be aligned with theintroduction of the zero-order waveplates 232, 270 discussed above inconnection with FIG. 2B.

[0056]FIG. 4A and FIG. 4C are top and side hardware block views of theembodiment of the optical interleaver shown in FIG. 3A. The polarizationbeam splitting cells shown in FIGS. 5-6 form the fundamental andharmonic filters of the single filter stage. The interleaver has 3 ports102, 188, 198 which couple with the fundamental filter cell 322 viacorresponding port couplers. The port coupler for port 102 includes:collimator 212 with a lens, beam splitter/combiner 214, and waveplates216. The port coupler for port 188 includes: collimator 482 with a lens,beam splitter/combiner 484, and waveplates 486. The port coupler forport 198 includes: collimator 492 with a lens, beam splitter/combiner494 and waveplates 496. In operation as an optical demultiplexer anoptical signal with odd and even channels modulated thereon enterscollimator 212 via port 102 which may be an optical fiber. The lenscollimator 212 may be a Graded Index of Refraction (GRIN) or other lenssystem. The lens focuses/collimates light depending on the propagationdirection to/from the beam splitter/combiner 214. The beamsplitter/combiner may be fabricated from a birefringent crystal with anoptic axis oriented to effect a walk-off of the optical signal ontowaveplates 216. The waveplates are zero-order waveplates and have theiroptical axis oriented to effect a linearization of the polarizationvectors of the two rays formed by the beam splitter/combiner.

[0057] The linearly polarized rays are then introduced into thefundamental filter cell which includes a polarization beam splittingcell 322 which operates as the fundamental filter and a zero-order halfwaveplate 124. In the embodiment shown, the fundamental filter operatesas a narrowband full/half waveplate or half/full waveplate for the oddset of channels and the even set of channels. The angle of thepolarization vector for the linearly polarized rays with respect to thepolarization axis (see FIG. 5) of the fundamental filter cell determinesthe coupling of the optical signal onto the fast and slow paths in thefundamental filter cell. The harmonic filter cell 340 optically coupleswith the fundamental filter cell and imposes a higher order harmonic onthe optical signals processed in the fundamental filter. The angle ofthe polarization vector for the linearly polarized rays from thefundamental cell with respect to the polarization axis of the harmonicfilter cell determines the coupling of the optical signal onto the fastand slow paths in the harmonic filter cell.

[0058] The retro reflector 160 then couples these split optical signalsonto the second optical processing leg 422 back into the first stage,i.e. the harmonic filter cell 240 and the fundamental filter cell wherethey will be further isolated. The beam splitter/combiner 250 mayintersect either or both of the optical processing legs 420, 422. Thezero-order half waveplate 124 is optically coupled to the fundamentalfilter 322 on one of the optical processing legs, e. g. the opticalprocessing leg 422, to effect a substantial reduction of chromaticdispersion of the demultiplexed odd and even channels. In an alternateembodiment of the invention the zero-order half waveplate may beintegrated with the fundamental filter, on either of the opticalprocessing legs 420, 422. The fundamental filter beam benders 272directs both odd and even channel optical signal outputs tocorresponding ones of beam benders 280 and 290 for redirection via thecorresponding port coupler components 482-486 and 492-496 to thecorresponding port 188 and 198 respectively. In operation as amultiplexer the propagation path between the ports 198, 188 and port 102is reversed. FIGS. 4A and 4C also show in dashed lines the zero-orderwaveplates 232 and 270 which allow the alignment of external features ofthe port couplers, fundamental filter cell and harmonic filter as shownin FIG. 3B.

[0059]FIG. 4B is a polarization diagram showing polarization vectorsalong the first and second leg 420, 422 respectively of the opticalprocessing loop formed within the embodiment of the optical interleavershown in FIG. 3A. The polarization diagrams are shown in views atvarious locations along the z-axis looking in the negative z direction.Polarization diagram 400 corresponds with the polarization states withinthe lenses of collimators 212, 482, and 492 for the polarization vectorsfor the optical signals entering/exiting ports 102, 188, and 198respectively. Polarization diagram 402 corresponds with the polarizationstates within the beam splitter/combiners 214, 484 and 494 for thepolarization vectors for the optical signals entering/exiting ports 102188, and 198 respectively. Polarization diagram 404 corresponds with thepolarization states within the waveplates 216, 486, and 496.Polarization diagram 406 corresponds with the polarization states withinthe fundamental filter 320 on the first and second optical processinglegs 420, 422. Polarization diagram 408 corresponds with thepolarization states within the fundamental filter 340 on the first andsecond optical processing legs 420, 422. Polarization diagram 410corresponds with the polarization states within the splitter/combiner250 on the first and second optical processing legs 420, 422.

[0060]FIG. 5 is an isometric view of a polarization beam splitting cellutilized in the embodiment of the optical interleaver shown in FIGS.3A-B. The optical filter cell employs couplers with polarizationdependent beam splitting to couple light onto a pair of delay paths.This polarization beam splitting cell is utilized in the embodiments ofthe invention shown in FIGS. 3A-B and 4A-B to form the fundamentalfilter 322 and the harmonic filters 340. The optical filter cellincludes couplers employing polarization dependent beam splittingbetween a pair of delay paths. Each coupler transmits and reflects lightdepending on the input properties of the light. In the embodiment of theinvention shown in FIG. 5A, each coupler is polarization sensitive andincludes “P” and “S” polarization axes orthogonal to one another. Afirst coupler is positioned in the propagation path of incomingpolarized light and transmits and reflects components of incomingpolarized light aligned with the “P” and “S” polarization axis of thecoupler respectively. Light transmitted and reflected by the couplerfollows two distinct delay paths, one for transmitted light and theother for reflected light. Where incoming light is orthogonallypolarized, the first coupler provides configurable amounts of couplingand cross-coupling of each of the orthogonal polarization vectors of theincoming light with either of the pair of delay paths. A second couplerpositioned at a location where the two distinct delay paths intersectreverses the process and re-aligns light with orthogonal polarizationvectors onto a common propagation axis.

[0061] The polarization beam splitting cell 322 is shown within an “x,y, z” or Cartesian coordinate system. The cell includes opposing opticalpolarization beam splitters 510, 530 displaced from one another alongthe z-axis with the optical element(s) 520A-B covering the span betweenthe splitters. Polarization beam splitter 510 is shown with a reflector512 and a polarization dependent beam splitter 514 displaced from eachother in a direction defined by the y-axis. Polarization beam splitter530 is shown with a reflector 532 and a polarization dependent beamsplitter 534 displaced from each other in a direction also defined bythe y-axis. The polarization dependent beam splitters have “S”polarization axes which are aligned, in the orientation of the cell thatis shown, parallel with the x-axis. The “P” polarization axis of eachpolarization dependent beam splitter is orthogonal to the “S” axis, i.e.aligned parallel with the 514, 534 need not be at 45 degree angles withrespect to incident optical signals, and in many implementations are atother angles, usually larger than 45 degrees. In some exampleembodiments, reflectors 512, 532 and polarization dependent beamsplitters 514, 534 are at an angle of approximately 55 degrees withrespect to the incident optical signals, but a wide range of angles arepossible depending on the particular implementation.

[0062] Each polarization beam splitter 510, 530 may be fabricated fromtwo pairs of prisms (not shown). In this case, polarization beamsplitter 510 and the polarization dependent beam splitter 514 may beformed from a first pair of prisms at right or other complementaryangles to one another. These may be affixed to one another, e.g.cemented, to minimize wave front distortion. The hypotenuse of one ofthe prisms is coated with a multi-layer dielectric polarizing beamsplitter coating. The prisms are then affixed to one another, to form afirst rectangle, the exterior surfaces of which may be antireflection(AR) coated to minimize surface reflection losses. A second pair ofprisms may be used to form the reflector 512. The hypotenuse of one ofthis second pair of prisms is coated with a reflective dielectriccoating, and cemented to the hypotenuse of the other of the second pairof prisms to form a second rectangle, the exterior surfaces of which mayalso be AR coated. The two rectangles formed by the two pairs of prismsmay then be affixed to one another to form the polarization beamsplitter 510. A similar technique may be used to fabricate the secondpolarization beam splitter 530.

[0063] Alternatively, polarization beam splitter 510, 530 may befabricated from two prisms 511, 515 or 531, 535 and a parallel plate513, 533 at right or other complementary angles to one another. Thesurface of the parallel plate that forms polarization dependent beamsplitter 514 may be coated with a multi-layer dielectric polarizing beamsplitter coating. The surface of the parallel plate that forms reflector512 also may be coated with a multi-layer dielectric polarizing beamsplitter coating or simply may be coated with a reflective dielectriccoating. In other embodiments, the surfaces of the prisms that affix tothe parallel plate may be coated with the appropriate coating. It shouldbe appreciated that the prism attached to reflector 512 may be omittedif the parallel plate, as opposed to prism, is coated with themulti-layer dielectric polarizing beam splitter or reflective coating.The parallel plate and prisms may be affixed to one another with anoptical bond (i.e., optical contact, epoxy free), and the exteriorsurfaces of polarization beam splitter 510 AR coated to minimize surfacereflection losses. A similar technique may be used to fabricate thesecond polarization beam splitter 530.

[0064] Other variations on the cell are discussed in U.S. patentapplication Ser. No. 09/944 037 filed on Aug. 31, 2001 and entitled:“METHOD AND APPARATUS FOR AN OPTICAL FILTER” as well as U.S. patentapplication Ser. No. 09/879026 filed on Jun. 11, 2001 and entitled:“METHOD AND APPARATUS FOR AN OPTICAL FILTER.”

[0065] In FIG. 5A the optical signals associated with the first andsecond legs of the optical loop are shown. Beams 542, 544 are shownpropagating through the filter cell along the first leg of the opticalloop and exiting the filter cell as beams 546, 548 respectively. Theirpolarization states on entry and exit from the fundamental cell areshown in FIGS. 5D-5E respectively. Beams 550, 552, 554, 556 are shownpropagating through the filter cell in the opposite direction along thesecond leg of the optical loop and exiting the filter cell as beams 558,560 562 564 respectively. Their polarization states on entry and exitfrom the fundamental cell are shown in FIGS. 5D-5E respectively. Thecell filters light bi-directionally. For purposes of illustrationpolarized light is shown entering the cell in a negative direction alongthe z-axis on the first leg of the optical processing loop and in apositive direction along the z-axis on the second leg of the opticalprocessing loop. Propagation in the opposite direction is alsosupported. The cell is also highly directional so that light propagatingin one direction is independent of the light propagating in the reversedirection.

[0066]FIG. 5B shows the fast and slow delay paths θ_(P1) and θ_(S1)within the polarization beam splitting cell shown in FIG. 5A. Beam 542is split by beam splitter 514 into a pair of slow/fast delay paths 548,550. Reflectors 512, 532 reflect the optical signals on delay path 548back to the splitter 534 where they are recombined with the opticalsignals on delay path 550. Similar optical processing is applied to beam544. The amount of delay on the P and S delay paths are θ_(P1) andθ_(S1) respectively. The delay of each path is determined by itscorresponding optical path length. The optical path length of each pathis the sum of the product of physical dimension and the index ofrefraction of all the optical elements on each of the two distinct S andP delay paths 548, 550 respectively. Optical element(s) 520A-B cover thespan between the splitters on the P delay paths. These optical elementshave a different optical pathlength than the optical elements, solid,liquid, gas, plasma, which make up the S path. The delay difference forthe cell is proportional to the difference in the optical path lengthsbetween the P and S delay paths. The delay difference exhibits itself inthe optical properties of the output beam 546. That output beam exhibitsthe interference pattern produced by the re-coupling of the P and Sdelay paths by the second of the polarization beam splitters 534 into asingle output beam.

[0067] The output beam includes orthogonal polarization vectors shownwith a square and a circle. Each contains complementary periodic stopbands and pass bands of the other with center wavelengths the spacingbetween which is inversely related to the delay difference between the Pand S delay paths. In other words the larger the delay difference thesmaller the wavelength spacing which the optical filter cell canresolve.

[0068]FIG. 5C is an isometric view of a linearly polarized opticalsignal in relation to the polarization axis of the polarization beamsplitting cell shown in FIG. 5A. Polarized light from beam 542 forexample, will couple with both the P and S axis of the coupler 514, apolarization beam splitter, in amounts which corresponded with therelative angular rotation between the polarization vector(s) of thepolarized input and the orthogonal P and S polarization axis of the beamsplitter. The component of a polarized input which projects onto the Spolarization axis of the beam splitter will be reflected by the beamsplitter. The component of a polarized input which projects onto the Ppolarization axis of the beam splitter will be transmitted by the beamsplitter.

[0069] The polarized light beam 542 may be arbitrarily, circularly orlinearly polarized. In the example shown, beam 542 is linearly polarizedwith a polarization vector 570 at an angle φ₁ with respect to the “S1”polarization axis 516 of the cell. As the beam 542 enters the cell it isaccepted onto either of two distinct S and P delay paths 548, 550respectively. These delay paths link the polarization dependent beamsplitters 514, 534. The amount of light that is coupled onto eitherdelay path is determined by the angle φ₁ of the incoming beam vectorwith respect to the S polarization axis of the cell.

[0070] In the example shown, light from polarization vector 570 inamounts proportionate to sin²(φ₁) and cos²(φ₁) will couple to the P andS delay paths respectively. Rotation of the cell about the propagationpath, e. g. the z-axis, of the beam 542 can be used to vary the couplingpercentages or ratios between the incoming light and the P and S delaypaths. Similar considerations apply for beams 550-556 on the second legof the optical processing loop. Where incoming light includes orthogonalpolarization vectors the coupling of either vector will be determined byprojecting that vector onto the P and S polarization axis of thepolarization beam splitter as well. The polarization beam splitters 514,534 thus serve as couplers which provide configurable amounts ofcoupling and cross-coupling of incoming beams with either of the pair ofdelay paths.

[0071] FIGS. 5D-E show polarization diagrams for opposing sides of thepolarization beam splitting cell shown in FIG. 5A. Polarization diagram502 shows an embodiment of the possible polarization states for beams542, 544 entering the filter on the first leg of the optical loop andfor beams 558, 562 exiting the filter from the second leg of the opticalloop. Polarization diagram 504 shows representative polarization statesfor beams 546, 548 exiting the filter on the first leg, and for beams552, 556 entering the filter on the second leg of the optical loop. Theoptical polarization beam splitter/displacer and retro reflector whichform the optical loop between the first and second legs are not shown(see FIGS. 3A-B). The vector with a square at the end contains passbands with center wavelengths at odd integer multiples of the periodicinterval established by the delay difference between the delay paths inthe filter. The vector with a circle at the end contains pass bands withcenter wavelengths at even integer multiples of the periodic intervalestablished by the delay difference between the delay paths in thefilter.

[0072] Beam 542 enters the first leg with multiplexed odd and evenchannels, and exits the filter with the odd and even channelsdemultiplexed onto corresponding one of the two orthogonal outputvectors which make up beam 546. The optical polarization beamsplitter/combiner/displacer 250, 251 (see FIGS. 3A-B) splits theseorthogonal component vectors into beams 550, 554 which are reflected byretro reflector 160 (see FIGS. 3A-B) and passed along the second leg ofthe optical processing leg including the portion of the second leg whichintersects filter cell 322. On the second pass through the fundamentalcell provided by the second leg any vestigial odd components in the evenchannels and even components for the odd channels are removed.

[0073] Without an offset in the FSR of the portion of the first andsecond legs of the optical loop which intersect the fundamental filtercell, chromatic dispersion will be additive rather than complementary.Complementary chromatic dispersions on the first and second legs aredesirable because they improve signal integrity. The amount ofimprovement in signal integrity is determined by the extent to whichdispersions are at any frequency of equal and opposite sign (see FIGS.7A-B). The offset in FSRs may be achieved by coupling the cell 322 witha zero-order waveplate as shown in FIGS. 3A-B or within the polarizationbeam splitting cell 322 itself. In the former case the polarization beamsplitting cell and a zero-order half waveplate make up the fundamentalfilter cell. The polarization beam splitting cell is the fundamentalfilter portion of the fundamental filter cell and operates as anarrowband full/half or half/full waveplate for the odd and evenchannels respectively. The zero-order waveplate completes thefundamental filter cell by coupling with the fundamental filter on oneof the two legs of the optical loop and effecting phase retardations ofodd integer multiples of substantially half a wavelength for each centerwavelength of a corresponding channel in both the odd the odd set ofchannels and the even set of channels. In the latter case thefundamental filter and the zero-order half waveplate are integrated withone another in a single polarization beam splitting cell. In thisembodiment of the invention, the optical element(s) 520A-B which coverthe span between the polarization beam splitters exhibit optical pathlengths, the difference of which on the first and second legs results inthe phase retardations of odd integer multiples of substantially half awavelength for each center wavelength of a corresponding channel in boththe odd set of channels and the even set of channels.

[0074]FIG. 5F shows polarization beam splitting cell 322F verticallymounted on a base 505. Typically, polarization beam splitters 510, 530and optical elements 520 are mounted on base 505 with an epoxy. However,differences in thermal expansion between the polarization beamsplitters, optical elements, epoxy or other adhesive/cement, and thebase cause the base 505 to bend in the θ direction, which, as shown inFIG. 5H, is extremely responsive in terms of producing wavelengthchanges in the optical signals passing through the cell.

[0075] In contrast, FIG. 5G shows polarization beam splitting cell 322Ghorizontally mounted on a base 505. In other words, optical signals passthrough polarization beam splitting cell 322G substantially parallel tobase 505. With respect to a polarization beam splitting cell or otheroptical component, substantially parallel should be interpreted suchthat optical signals pass through the faces 575, 577, 585, 587. Heretoo, polarization beam splitters 510, 530 and optical elements 520G aremounted on base 505 with an epoxy or other adhesive/cement. However, inFIG. 5G differences in thermal expansion between the polarization beamsplitters, optical elements, epoxy, and base cause the base 505 to bendin the φ direction, which, as shown in FIG. 5G, is relativelyunresponsive in terms of producing wavelength changes in the opticalsignals passing through the cell. Accordingly, when mounted horizontallyto base 505 as illustrated in FIG. 5G, the polarization beam splittingcell 322G exhibits greater thermal stability than when mountedvertically as illustrated in FIG. 5F. Similar to the filter cellsdiscussed above in connection with FIGS. 2B and 3B, waveplates can beinserted in order to rotate optical signal polarizations appropriatelyfor the horizontal mounting of polarization beam splitting cell 322Nand/or other optical components.

[0076] For simplicity, FIG. 6A is an isometric view of a multi-cellimplementation of the polarization beam splitting cell of FIG. 5Autilized in the embodiment of the optical interleaver shown in FIG. 3A.Of course as described above, other polarization beam splitting cells,such as those illustrated in FIG. 5F could be used as well. One or moreoptical elements 520 are shown as a single element spanning the P pathbetween the two splitters 510, 530. This single element presents thesame optical pathlength on both the first and second leg of the opticalprocessing loop. Two cells 322 and 340 are shown coupled to one anotherin series. Sequentially coupling cells allows an optical filter toexhibit a more complex transfer function than the simple sinusoidaloutput provided by the single cell shown in FIG. 5A. In this example thedelay paths provided by harmonic cell 340 and their delay difference arelarger than the delay paths and delay difference provided by thefundamental cell 322. This result can be achieved either by fabricatingcell 340 from the same optical elements as cell 322 with an increase inthe physical length of the elements or by fabricating cell 340 fromoptical elements with higher indices of refraction than those of cell322 thus maintaining the same form factor for both cells.

[0077] The combination of first cell and subsequent cells can be lookedat as establishing by the difference between their delay paths thefundamental sinusoidal harmonic for the sequence and higher orderharmonics. In an embodiment of the invention this objective is achievedby designing one of the cells in the sequence with a FSR correspondingwith the desired fundamental harmonic and with others of the cellsdesigned with FSRs which are integer fractions of the base FSR. Thecoefficients or amplitude of each harmonic are provided by varying thecoupling ratio percentage, coefficients between a polarized input to acell and the “P” and “S” polarization axes of the cell as provided bythe corresponding polarization beam splitter. The coupling coefficientsare varied by tilting of a cell about the propagation path of apolarized input to each cell.

[0078] Cell 322 includes the components described above in connectionwith FIG. 5A. Between cell 322 and 340 on the second optical processingleg the zero-order half waveplate 124 is shown. Cell 340 includescouplers 614, 634 employing polarization dependent beam splitting linkedby a pair of delay paths 650 and 646 648, 652. The cell 340 includesopposing polarization beam splitters 610, 630 displaced from one anotheralong the z-axis with one or more optical elements 620 (shown as asingle optical element) covering the span between the splitters.Polarization beam splitter 610 is shown with a reflector 612 and apolarization dependent beam splitter 614 displaced from each other in adirection defined by the y-axis. Polarization beam splitter 630 is shownwith a reflector 632 and a polarization dependent beam splitter 634displaced from each other also in a direction defined by the y-axis. Thepolarization dependent beam splitters have “S” polarization axes whichare aligned with one another. Between the couplers one or more opticalelements 620 is shown. The various components are shown on top of base606.

[0079] Only one of the beams on one of the legs of the opticalprocessing loop is shown. That polarized beam 542 has, in the exampleshown, a linearly polarized input vector (see FIG. 6B). This beam entersthe cell 322 where it reflected and transmitted by polarization beamsplitter 514 onto one end of the pair of delay paths θ_(S1) and θ_(P1).At the opposite end of the delay paths reflection and transmission bythe polarization beam splitter 534 produces a common output beam 546which exits the cell on the first leg and proceeds directly to theharmonic cell 340, without intersecting the zero-order half waveplate124.

[0080] On entering the harmonic cell, beam 546 is reflected andtransmitted by polarization beam splitter 614 onto one end of the pairof delay paths θ_(S2) and θ_(P2). At the opposite end of the delaypaths, reflection and transmission by the polarization beam splitter 634produces a common output beam 546N with orthogonal polarization vectorswith odd and even channel components (see FIG. 6C). The process can beextended with more harmonic filters to form a more complex opticalfilter transfer function.

[0081] FIGS. 6B-C show polarization diagrams for opposing ends of thepolarization embodiment of the possible polarization states for beam 542entering the filter on the first leg of the optical loop. Polarizationdiagram 604 shows representative polarization states for beam 546Nexiting the last filter cell 340 on the first leg or the opticalprocessing loop. The splitter and retro reflector which form the opticalloop between the first and second legs are not shown (see FIGS. 3A-B).The vector with a square at the end contains pass bands with centerwavelengths at odd integer multiples of the periodic intervalestablished by the delay difference between the delay paths in thefilter. The vector with a circle at the end contains pass bands withcenter wavelengths at even integer multiples of the periodic intervalestablished by the delay difference between the delay paths in thefilter.

[0082] Beam 542 enters the first leg with multiplexed odd and evenchannels, and exits the filter with the odd and even channelsdemultiplexed onto corresponding one of the two orthogonal outputvectors which make up beam 546N. The optical polarization beamsplitter/combiner/displacer 250 (see FIGS. 3A-B) splits these orthogonalcomponent vectors into beams which are reflected by retro reflector 160(not shown, but see FIGS. 3A-3B) and passed along the second leg of theoptical processing leg back through cells 340 124, and 322 in adirection opposite to the propagation direction in the first leg. On thesecond pass through the fundamental cell, any vestigial odd componentsin the even channels and even components for the odd channels areremoved.

[0083]FIG. 6D is a side elevation view of the delay paths of themulti-cell implementation shown in FIG. 6A. The delay introduced intolight passing along any delay path is a function of the optical pathlength of the optical elements which comprise the delay path. Opticalpath length “L” of an optical element is expressed as the product of thephysical distance “d” traversed by a beam propagating through theelement multiplied by the index of refraction “n” of the element. Wheremultiple optical elements are involved, the individual contributions tothe optical path length from the individual elements are summed. Forpurposes of the current invention, optical elements include: a vacuum, agas, a liquid, a solid or a plasma along the propagation path. The indexof refraction of a medium identifies the ratio of the speed of light ina vacuum to that of light in the medium. Where the optical path lengthvaries as here between two delay paths, one path is said to befaster/slower than the other and there is said to be a delay differencebetween the two.

[0084] Beam 542 propagates through the first cell 322 across delay pathsθ_(P1) and θ_(S1) and through the second cell 340 across delay pathsθ_(P2) and θ_(S2). Delay path θ_(P1) comprises optical elements definedby optical path length L₁₅-L₁₇. Delay path θ_(S1) comprises opticalelements defined by optical path lengths L₁₀-L₁₄. Delay path θ_(P2)comprises optical elements defined by optical path length L₂₅-L₂₇. Delaypath θ_(S2) comprises optical elements defined by optical path lengthsL₂₀-L₂₄. In the embodiment shown, the optical elements defined byoptical path lengths L₁₂ and L₂₂ include air/gas/vacuum. The remainingoptical elements may be fabricated from various types of optical glassincluding: BKx, fused silica, SFx. By proper design of delay paths, thefundamental and higher order harmonics for the optical filter may beestablished.

[0085] The delay for the delay paths θ_(P1) and θ_(S1) in the firstfilter 322 are expressed as a function of the optical path lengths ofeach path in the following Equations 4-5 respectively. $\begin{matrix}{\theta_{S1} = {( {2\quad \pi \frac{v}{c}} )( {\sum\limits_{i = 1}^{i = I}\quad {d_{i}n_{i}}} )}} & {{Equation}\quad 4} \\{\theta_{P1} = {( {2\quad \pi \frac{v}{c}} )( {\sum\limits_{j = 1}^{j = J}\quad {d_{j}n_{j}}} )}} & {{Equation}\quad 5}\end{matrix}$

[0086] where c and ν are the frequency and velocity of light in freespace and where I and J are the number of optical elements which make upthe delay paths with delays θ_(S1) and θ_(P1) respectively. For each ofthe i optical elements: vacuum, gas, plasma, liquid or solid which makeup the delay path θ_(S1) the i^(th) element has a physical length d_(i)and an index of refraction n_(i). For each of the J optical elements:vacuum, gas, plasma, liquid or solid which make up the delay pathθ_(P1), the j^(th) element has a physical length d_(j) and an index ofrefraction n_(j). Optical elements include the optical coatingsassociated with polarization or intensity dependent beam splitters,which also contribute to optical pathlength and phase accumulations.

[0087] The delay difference between the two paths is expressed inEquation 6. $\begin{matrix}{{\theta_{S1} - \theta_{P1}} = {( {2\quad \pi \frac{v}{c}} )( {{\sum\limits_{i = 1}^{i = I}\quad {d_{i}n_{i}}} - {\sum\limits_{j = 1}^{j = J}\quad {d_{j}n_{j}}}} )}} & {{Equation}\quad 6}\end{matrix}$

[0088] The delay difference for the cell is proportional to thedifference in the optical path lengths between the S and P delay paths.Similar considerations apply in determining the delays and delaydifferences for the pair of delay paths in the second cell 340.

[0089] The optical path length difference between the two delay paths ina cell corresponds inversely with the free spectral range (FSR)generated by the cell as evidenced in the orthogonal vector componentsof the output beam from the cell. This relationship is set forth in thefollowing Equation 7. $\begin{matrix}{{FSR} = {( \frac{c}{{L_{I} - L_{J}}} ) = {( \frac{c}{{{\sum\limits_{i = 1}^{i = I}\quad {d_{i}n_{i}}} - {\sum\limits_{j = 1}^{j = J}\quad {d_{j}n_{j}}}}} ) = ( {2\pi \frac{v}{\theta_{S} - \theta_{P}}} )}}} & {{Equation}\quad 7}\end{matrix}$

[0090] where L_(I) and L_(J) are the total optical path length of the Iand J elements which make up the corresponding delay paths θ_(S) andθ_(P).

[0091] For an optical interleaver the FSR should be a constant perhapsequal to the channel spacing between adjacent odd or even channels,e.g., 100 GHz. Using Equation 7 the delay difference required togenerate this result can be determined, and from it a solution to theoptical path lengths for each of the delay paths.

[0092]FIG. 6E is a side elevation view of the variable coupling betweencells of the multi-cell implementation shown in FIG. 6A. Coupling isused to control the amount an input of polarized light that will beprojected onto the S and P delay paths of a corresponding cell. Threecoupling views 660, 662 and 664 are shown at appropriate locations atthe input to cell 322, the interface between cells 322 and 340 and atthe output of cell 340 respectively. Only one of beams 542 on one of theoptical processing legs, e. g. the first optical processing leg, areshown. The three views 660-664 are taken at the stated locations alongthe z-axis looking in the positive z direction along the propagationpath of the input beam 542. In the first of the coupling views 660, thepolarized input is shown with a single input vector “I” and theorthogonal polarization axes PI and SI of the first cell 322 are shown.The input I may include orthogonal input vectors. The amount of lightthat is coupled onto either delay path in the first cell is determinedby the angle θ₁ of the incoming beam vector with the S polarization axisof the cell. In the example shown light from beam 542 will couple to theP and S delay paths in amounts proportionate with the sin²(φ₁) and thecos²(φ₁) of the angle φ₁ between the vector of the beam and the P and Saxes. Rotation of the cell about the propagation path of the beam 542can be used to vary the coupling percentages or ratios between theincoming light and the P and S delay paths. In the next coupling view662, the beam 546 from cell 322 is coupled with cell 340. The orthogonalpolarization vectors P₁, S₁ present in the output of the fundamentalcell 322 are shown along with the orthogonal polarization vectors P₂, S₂which are defined by the coupler of the next cell in the sequence, i.e.harmonic cell 340. The amount of light that is coupled onto either delaypath in the second cell is determined by the angle φ₂ between the twosets of orthogonal vectors for beam 546 and the P and S axes of cell340. The last coupling view 664, shows both the orthogonal polarizationvectors P₂, S₂ present in the output of the second cell along with asecond set of orthogonal polarization vectors P₀, S₀. This lastorthogonal vector set is used to represent the optical polarization beamsplitter/combiner/displacer 250 (see FIG. 3A) used to separate theorthogonal vectors within the single output beam into two discrete beams(not shown). The amount of light coupled onto the output beams isdefined by the angle φ₃ between the two sets of orthogonal vectors.

[0093]FIG. 6F shows the individual transforms associated with each ofthe four delay paths on one of the two optical processing legs throughthe two cell sequence shown in FIG. 6A. FIG. 6F shows the individualtransforms 688 associated with each of the four distinct delay pathsfrom the input of beam 542 to the output of beam 546N. The number ofdiscrete paths in a multi-cell sequence of N cells with two delay pathsbetween each equals 2^(N). For two cells there are 2² or 4 discretepaths between an input and an output. The first of these paths is alongdelay paths θ_(S1) and θ_(S2) in the first cell 322 and the second cell340 respectively. The second of these paths is along delay paths θ_(S1)and θ_(P2). The third of these paths is along delay paths θ_(P1) andθ_(S2). The fourth of these paths is along delay paths θ_(P1) andθ_(P2). The transfer function for the optical filter in single orsequential cell embodiments is the sum of the individual transferfunctions associated with each discrete path from input to output.Transfer functions: 688, 690, 692, 694 are shown for the 1^(st) to4^(th) paths discussed above. Each transfer function includes two terms696-698. The first term 696 corresponds to a coefficient in a Fourierseries with the coefficient magnitude proportional to the product of thecoupling or cross coupling coefficients along the particular path. Thesecond term 698 corresponds to the frequency component associated withthat coefficient. The frequency component corresponds with the sum ofthe delays along a corresponding path. This in turn corresponds with theoptical path lengths along each path. The sum of all the transferfunctions forms a truncated Fourier series which fully defines theoptical filter.

[0094] In an embodiment of the invention in which the opticaltelecommunications grid includes channels spaced apart by 50 GHz, amulti-cell design includes a fundamental cell of 100 GHz FSR and aharmonic cell of 50 GHz FSR to form polarization type square top combfilters. This filter can split an optical stream with 50 GHz channelspacing into two separate optical streams with odd and even 100 GHzchannel spacing respectively or combine two optical streams with 100 GHzodd and even channel spacing respectively into a single optical streamwith 50 GHz channel can spacing. The 1^(st) angle φ₁ can besubstantially equal to 45 degrees and the 2^(nd) angle can besubstantially equal to (45+15) degrees. Similarly, a first cell of 100GHz FSR and a second cell of 50 GHz FSR can be used to form an intensitytype of square top comb filters. The 1^(st) splitting ratiosubstantially equals 50/50% and the 2^(nd) splitting ratio substantiallyequals cos²(45°+15°)/sin²(45°+15°). In a multi-cell embodiment a squaretop filter function may be achieved by choosing one cell with the baseFSR and remaining cells with FSRs of integer fractional multiples of thebase FSR.

[0095] Further teachings on sequentially coupled optical filter cellsmay be found in either of the two following references. See E. Harris etal., Optical Network Synthesis Using Birefrinent Crystals, JOURNAL OFTHE OPTICAL SOCIETY OF AMERICA, VOLUME 54, Number 10, October 1964 for ageneral discussion of transfer functions related to birefringentcrystals. See C. H. Henry et al. U.S. Pat. No. 5,596,661 entitled“Monolithic Optical Waveguide Filters based on Fourier Expansion” issuedon Jan. 21, 1997 for a general discussion of transfer functions relatedto wave guides.

[0096] Passive Thermal Stabilization

[0097] The typical application of optical filters constructed using theabove techniques is an optical interleaver. In order for thatinterleaver to function properly it must create the desired stop bandsand pass bands for the odd and even channels which it separates. Forcurrent telecommunication applications the filter would be designed witha constant FSR perhaps equal to the channel spacing, i.e., 100 GHz. Anoptical filter with this FSR would generate the required stop bands andpass bands in each of the orthogonal polarization vectors present on theoutput. One of the orthogonal output vectors would contain the passbands associated with the center wavelengths of the odd channels. Theother of the orthogonal output vectors would contain the pass bandsassociated with the center wavelengths of the even channels.

[0098] Temperature variations in a interleaver that may effect theperformance may result from the environment or from the powertransmitted through the interleaver. This can result in the periodic oddand even pass bands generated by the optical filter moving out ofalignment with the selected grid, i.e., the ITU grid. This is primarilybecause the center wavelength of a pass band slips with temperature.This misalignment results in attenuation of signal strength, cross talkand ultimately loss of transmission/reception capability until theoptical filter returns to its original temperature. In practicetherefore, the optical filters and interleavers fabricated there frommust be thermally stable across a range of temperatures.

[0099] One solution is to flatten the pass bands of the filter. Multicell filter designs such as those discussed above allow the pass bandsto exhibit higher order harmonics in the form of non-sinusoidal passband profiles, a.k.a. “flat tops” (see FIG. 11). The close spacingbetween the channels in a WDM makes it desirable to design a WDM withflat pass bands in order to increase the error tolerance to temperatureinduced shifts in the pass bands. Even with flat top filter profiles,however, temperature stabilization is still required due to the precisetelecommunication channel spacing.

[0100] A further solution is to actively stabilize the temperature ofthe interleaver using a heater or cooler and a closed loop feedback oftemperature or wavelength. This solution can be expensive and mayincrease the form factor of the interleaver. Nevertheless, the currentinvention may be practiced with active temperature stabilization. Apossible benefit to active temperature stabilization is that the opticalelements which make up each pair of delay paths may all be fabricatedfrom a common medium with identical indices of refraction and thermalexpansion coefficient.

[0101] Although capable of being utilized in systems with activetemperature stabilization, the current invention is capable of providingtemperature stability for the optical filters without active temperaturecontrol where appropriate. This greatly enhances the precision of theinterleavers or systems fabricated there from and reduces system cost.The current invention is capable of providing passive temperaturestabilization of an optical interleaver, through proper selection anddesign of the optical elements which form each pair of delay paths sothat the delay difference for each pair of delay paths and hence thesystem as a whole remain constant. Since the delay difference isdirectly related to the difference in the optical path lengths thisinvention provides thermal stabilization of the delay difference. In anembodiment of the invention either the birefringent or the polarizationbeam splitting filters may be fabricated with at least one of the delaypaths having two optical elements, each of which exhibits a differentoptical path length response to temperature. Typically, this takes theform of optical elements with different thermal optic coefficients.

[0102] The system is designed so that d(L_(I)-L_(J))/dT equalssubstantially zero. This latter condition is satisfied when thederivative of the denominator in Equation 7 substantially equals zero asset forth in the following Equation 8: $\begin{matrix}\begin{matrix}{\frac{( {L_{I} - L_{J}} )}{T} = \frac{( {{\sum\limits_{i = 1}^{i = I}\quad {d_{i}n_{i}}} - {\sum\limits_{j = 1}^{j = J}\quad {d_{j}n_{j}}}} )}{T}} \\{{= {{\sum\limits_{i = 1}^{i = I}( \quad {{d_{i}\beta_{i}} + {\alpha_{i}n_{i}d_{i}}} )} - {\sum\limits_{j = 1}^{j = J}\quad ( \quad {{d_{j}\beta_{j}} + {\alpha_{j}n_{j}d_{j}}} )}}}\quad} \\{\approx 0}\end{matrix} & {{Equation}\quad 8}\end{matrix}$

[0103] where α_(j) and α_(j) are the thermal expansion coefficients foreach optical element which form the S and P delay paths respectively ineach cell and where β_(i) and β_(j) are the thermal optic coefficientsfor the temperature induced change in the refractive index for eachelement in the S and P delay paths respectively.

[0104] The following Table 1 shows various relevant optical parametersfor some optical media which may be used to fabricate the opticalelements which make up each pair of delay paths. TABLE 1 Fused @1550 nmVacuum Air BK7 SF5 Silica BaK1 LaSFN3 n 1 1.00027 1.50066 1.64329 1.44091.55517 1.77448 $\beta = {\frac{n}{t} \times 10^{- 6}}$

0 0* 0.907465 1.407 13.7 0.066 2.293 α× 10⁻⁶ 0 0* 5.1 8.2 0.052 7.6 6.2

[0105] The second row sets forth each material's refractive index at1550 nm. The change in refractive index n as a function of temperature βis set forth in the third row. Row 4 sets forth the coefficient ofthermal expansion a for the medium. The selection of physical length ofeach optical component can be determined by solving Equation 4 and 5together.

[0106] Further passive thermal stabilization may be achieved byhorizontally mounting a polarization beam splitting cell to a substrateas illustrated in FIG. 5G.

[0107] FIGS. 7A-B are graphs showing the complementary dispersionprofiles about a representative center frequency of one of the channelsfor an optical interleaver fabricated in accordance with the currentinvention. The complementary dispersion profiles result from the abovediscussed asymmetry in the fundamental filter between the opticalpathlengths along the portions of the first and second legs of theoptical loop which intersect the fundamental filter. FIG. 7A shows arepresentative dispersion profile where coupling of light onto fast andslow paths of either of the optical processing legs is in equalproportions. The dispersion profiles 700 and 702 for the first leg andthe second leg are shown relative to the substantially flat linecomposite dispersion 704. The flat line dispersion profile results fromthe broadband phase shift for the odd and even channel sets between thefirst and second optical processing legs in the fundamental filter cell.This phase shift of odd integer multiples of substantially half awavelength for each center wavelength of a corresponding channel in boththe odd set of channels and the even set of channels causes the oddchannel set and the even channel set to experience the fundamentalfilter cell as respectively a full/half waveplate and a half/fullwaveplate on the first and second legs of the optical loop within thefundamental filter cell. This phase shift is advantageous because itimproves the signal integrity associated with multiplexing andde-multiplexing telecom communications by reducing overall chromaticdispersion in each of the channels filtered by the interleaver.

[0108]FIG. 7B shows a representative dispersion profile where couplingof light onto fast and slow paths of either of the optical processinglegs is in un-equal proportions. The dispersion profiles 710 and 714 forthe first and second leg of the optical loop are shown relative to thecomposite dispersion 716. The composite dispersion exhibits somedeviation from the desired flat line response, but the tradeoff in termsof enhanced stop bands in the filter transform is appropriate for someapplications as will be shown in the following FIGS. 8A-E

[0109] FIGS. 8A-E are signal diagrams showing filter functions atvarious locations along the optical path of the interleaver shown inFIGS. 1-6. The signal diagrams shown in FIGS. 8A-B show the periodiccomb filter functions to which the even channels are exposed on thefirst and second legs of the optical processing loop respectively. Thefirst comb filter function to which the even channels are exposed on thefirst leg includes pass bands for the even channels interlaced withresidual components, or bleed through, of the odd channels and is shownin FIG. 8A. In the first leg, in this example the even channels aresubject to a phase retardation substantially equal to the incidentwavelength or integer multiples thereof. Thus there is a pass band 860for channel 10 and one for channel 12. The center frequency 864 for thepass band for channel 12 coincides with a selected order of the incidentwavelength, e.g., order 3875. Between the pass bands for the evenchannels there is a bleed through of the odd pass bands below the −10 dBlevel. The bleed through 862 for channel 11, as well as channels 9 and13 are shown. This bleed through results from asymmetric coupling oflight onto the fast and slow paths in amounts other than 50%/50%.

[0110] The coupling asymmetries in the first leg between the fast andslow paths of each filter cell are present in the second leg as shownfor the even channels in FIG. 8B. Because of the wavelength shift of λ/2or odd integer multiples thereof, in the optical pathlength differencebetween the portion of the first and second legs which intersect thefundamental cell, the even channels are subject to a second comb filterfunction different than that to which they were exposed in the firstsub-stage. This second comb filter function shown in FIG. 8B includesnarrow stop bands, and substantially attenuated bleed-through of the oddchannels. There is a pass band 866 for channel 10 and one for channel 12with a slight dip in the flat top. The center frequency 864 for channel12 coincides with a different selected order of the incident wavelength,e.g. order 3876, than was the case in the filter of the first sub-stageas shown in FIG. 8A.

[0111] The signal diagrams shown in FIGS. 8C-D show the comb filterfunctions to which the odd channels are exposed on the first and secondlegs of the optical processing loop respectively. In the first leg, inthis example the odd channels are subject to the second comb filterfunction with a wavelength shift of λ/2 or odd integer multiplesthereof. Thus there is a pass band 870 for channel 11 and one forchannels 9 and 13. The center frequency 864 for the pass band forchannel 12 coincides with a selected order of the incident wavelength,e.g. order 3875. The filter function for the odd channels in the firstsub-stage exhibits narrow stop bands, and substantially attenuatedbleed-through. The coupling asymmetries in the first leg between thefast and slow paths of each filter cell are present in the second leg.

[0112] As show in FIG. 8D the wavelength shift of λ/2 in the opticalpathlength difference between the portion of the first and second legswhich intersects the fundamental cell results in the odd channels alsobeing subject to a different, i.e. complementary filter function, tothat experienced in the first leg. The odd channels are exposed to thefirst comb filter function with a wavelength shift of λ/2 or odd integermultiples thereof. There is a pass band 874 for channel 11 and one forchannels 9, 13. Between the pass bands for the odd channels there is ableed through of the even pass bands below the −10 dB level. The bleedthrough 872 for channel 10, as well as channel 12 is shown. This bleedthrough results from asymmetric coupling of light onto the fast and slowpaths in amounts other than 50%/50%. The same coupling ratios used inthe first leg are applied in the second leg. The center frequency 864for the pass band for channel 12 coincides with a different selectedorder of the incident wavelength, e.g. order 3876, than was the case inthe fundamental filter on the first leg as shown in FIG. 8C.

[0113]FIG. 8E shows the composite performance for the interleaver forboth the odd and even channels. The pass band 810 for even channel 10 aswell as for channel 12 is shown. The pass band 812 for odd channel 11 aswell as for channels 9 13 are also shown. Each pass band exhibits steepside profiles and broad stop bands when compared with prior art designs.The pass band 812 for channel 11 is shown with a broad flat top 804 andwith broad pass bands 816, 818. Superimposed on the pass band 812 is askirt 820 representative of traditional pass band profiles. Bycomparison the current interleaver exhibits a significant improvement inthe pass band profiles it generates with relatively steeper sides andbroader stop bands. These improvements translate into increases in thesignal integrity of the telecommunications data handled by theinterleaver.

[0114] In alternate embodiments of the invention, the various filter,retro reflector and other elements of the optical interleaver may befabricated on a common semi-conductor substrate. The various components:reflectors, couplers, and optical elements may be fabricated using acombination of etching and deposition techniques well know in thesemi-conductor industry.

[0115] The foregoing description of preferred embodiments of theinvention has been presented for purposes of illustration anddescription. It is not intended to be exhaustive or to limit theinvention to the precise forms disclosed. Obviously many modificationsand variations will be apparent to practitioners skilled in this art.

We claim:
 1. A filter cell for filtering optical signals propagating oneach of two legs of an optical loop which intersects the filter cell,the filter cell operating as a full waveplate to a first set of one ormore optical signals and a half waveplate to a second set of one or moreoptical signals on a selected one of the two legs and as a halfwaveplate to the first set of one or more optical signals and a fullwaveplate to the second set of one or more optical signals on aremaining one of the two legs, the filter cell comprising: a base; afirst polarization beam splitter (PBS) oriented to split or combine thefirst and second sets of one or more optical signals depending onpolarization and propagation direction along the optical loop, the firstPBS being horizontally mounted to the base such that the optical signalspropagate substantially parallel to the base in order to improve thefilter cell's thermal stability when the base becomes deformed; one ormore optical components optically coupled to the first polarization beamsplitter and also mounted to the base; and a second PBS opticallycoupled to the first PBS and the one or more optical components to splitor combine the first and second sets of one or more optical signalsdepending on polarization and propagation direction along the opticalloop, the second PBS being horizontally mounted to the base such thatthe optical signals propagate substantially parallel to the base inorder to improve the filter cell's thermal stability, wherein the secondPBS is oriented to split when the first PBS is oriented to combine andthe second PBS is oriented to combine when the first PBS is oriented tosplit.
 2. A filter cell as recited in claim 1, further comprising a pairof delay paths including a fast delay path and a slow delay path.
 3. Afilter cell as recited in claim 2, wherein the first PBS and the secondPBS asymmetrically split and combine the optical signals between thefast delay path and the slow delay path depending on the opticalsignals' polarization.
 4. A filter cell as recited in claim 2, whereinthe first PBS and the second PBS symmetrically split and combine theoptical signals between the fast delay path and the slow delay pathdepending on the optical signals' polarization.
 5. A filter cell asrecited in claim 1, wherein the first PBS and the second PBS comprise atleast one prism and a parallel plate.
 6. A filter cell as recited inclaim 5, wherein at least one surface of the parallel plate is coatedwith a multilayer dielectric polarizing beam splitter coating.
 7. Anoptical interleaver for processing optical signals including a first setof one or more optical signals and a second set of one or more opticalsignals, the interleaver comprising: a base; a filter cell mounted tothe base for filtering optical signals propagating on each of two legsof an optical loop, the filter cell operating as a full waveplate to thefirst set of optical signals and a half waveplate to the second set ofoptical signals on the first leg, and as a half waveplate to the firstset of optical signals and a full waveplate to the second set of opticalsignals on the second leg, the filter cell comprising: a firstpolarization beam splitter (PBS) horizontally mounted to the base andoriented to split or combine the first and second sets of opticalsignals depending on polarization and propagation direction along theoptical loop; one or more optical components optically coupled to thefirst polarization beam splitter and also mounted to the base; and asecond PBS optically also horizontally mounted to the base and coupledto the first PBS and the one or more optical components to split orcombine the first and second sets of optical signals depending onpolarization and propagation direction along the optical loop; a retroreflector mounted to the base and optically coupled with the filter cellto reflect the optical signals from the first leg to the second leg ofthe optical loop; and an optical polarization beam displacer mounted tothe base and optically coupled between the filter cell and the retroreflector to split or combine the first and second sets of opticalsignals depending on polarization and propagation direction along theoptical loop.
 8. An optical interleaver as recited in claim 7, furthercomprising one or more prisms to optically couple a plurality of portsto the filter cell.
 9. An optical interleaver as recited in claim 8,further comprising one or more waveplates to optically couple the one ormore prisms and the plurality of ports to the filter cell.
 10. Anoptical interleaver as recited in claim 7, wherein the filter cellcomprises a fundamental filter cell.
 11. An optical interleaver asrecited in claim 10, further comprising a harmonic filter cell opticallycoupled to the fundamental filter cell and the optical polarization beamdisplacer to filter the optical signals on both legs of the optical loopwith a higher order harmonic.
 12. An optical interleaver as recited inclaim 11, further comprising a zero-order waveplate optically coupledbetween the harmonic filter cell and the fundamental filter cell torotate polarization vectors of the optical signals between thefundamental filter cell and the harmonic filter cell in order to alignthe fundamental filter cell and the harmonic filter cell with eachother.
 13. An optical interleaver as recited in claim 12, furthercomprising a zero-order waveplate optically coupled between the harmonicfilter cell and the optical polarization beam displacer to rotatepolarization vectors of the optical signals between the harmonic filtercell and the optical polarization beam displacer in order to align theharmonic filter cell and the optical polarization beam displacer witheach other.
 14. An optical interleaver as recited in claim 7, whereinthe filter cell further comprises a pair of delay paths including a fastdelay path and a slow delay path.
 15. An optical interleaver as recitedin claim 14, wherein the first PBS and the second PBS asymmetricallysplit and combine the optical signals between the fast delay path andthe slow delay path depending on the optical signals' polarization. 16.An optical interleaver as recited in claim 14, wherein the first PBS andthe second PBS symmetrically split and combine the optical signalsbetween the fast delay path and the slow delay path depending on theoptical signals' polarization.
 17. An optical interleaver as recited inclaim 7, wherein the first PBS and the second PBS comprise at least oneprism and a parallel plate.
 18. An optical interleaver for processingoptical signals including a first set of one or more optical signals anda second set of one or more optical signals, the interleaver comprising:a base; a fundamental filter cell mounted to the base for filtering afirst and second set of optical signals propagating on each of two legsof an optical loop, comprising: a first and second polarization beamsplitter (PBS), each horizontally mounted to the base and oriented tosplit or combine the first and second sets of optical signals dependingon polarization and propagation direction; and one or more opticalcomponents optically coupled between the first and second polarizationbeam splitters, and also mounted to the base; a first harmonic filtercell optically coupled to the fundamental filter cell and mounted to thebase for filtering the first and second set of optical signals with ahigher order harmonic, comprising: a first and second polarization beamsplitter (PBS), each horizontally mounted to the base and oriented tosplit or combine the first and second sets of optical signals dependingon polarization and propagation direction; and one or more opticalcomponents optically coupled between the first and second polarizationbeam splitters, and also mounted to the base; a retro reflector mountedto the base and optically coupled with the first harmonic filter cell toreflect the optical signals from the first leg to the second leg of theoptical loop; and an optical polarization beam displacer mounted to thebase and optically coupled between the harmonic filter cell and theretro reflector to split or combine the first and second sets of opticalsignals depending on polarization and propagation direction.
 19. Anoptical interleaver as recited in claim 18, further comprising one ormore prisms to optically couple each of a plurality of ports to thefilter cell.
 20. An optical interleaver as recited in claim 19, furthercomprising one or more waveplates to optically couple the one or moreprisms and each of the plurality of ports to the filter cell.
 21. Anoptical interleaver as recited in claim 18, further comprising a secondharmonic filter cell optically coupled to the fundamental filter celland the polarization beam displacer to filter the optical signals onboth legs of the optical loop with a second higher order harmonic. 22.An optical interleaver as recited in claim 21, further comprising awaveplate optically coupled between a first harmonic filter cell and thefundamental filter cell to rotate polarization vectors of the opticalsignals between the fundamental filter cell and the first harmonicfilter cell in order to align the fundamental filter cell and the firstharmonic filter cell with each other.
 23. An optical interleaver asrecited in claim 22, further comprising a waveplate optically coupledbetween a first harmonic filter cell and a second harmonic filter cellto rotate polarization vectors of the optical signals between the secondharmonic filter cell and the first harmonic filter cell in order toalign the second harmonic filter cell and the first harmonic filter cellwith each other.
 24. An optical interleaver as recited in claim 23,further comprising a waveplate optically coupled between a secondharmonic filter cell and the polarization beam displacer to rotatepolarization vectors of the optical signals between the second harmonicfilter cell and the polarization beam displacer in order to align thesecond harmonic filter cell and the polarization beam displacer witheach other.
 25. An optical interleaver as recited in claim 18, whereinthe fundamental and harmonic filter cells each further comprises a pairof delay paths including a fast delay path and a slow delay path.
 26. Anoptical interleaver as recited in claim 14, wherein at least one of thefirst and second PBS of the fundamental filter cell and the first andsecond PBD of the harmonic filter cell asymmetrically splits andcombines the optical signals between the fast delay path and the slowdelay path of the corresponding filter cell depending on the opticalsignals' polarization.
 27. An optical interleaver as recited in claim14, wherein at least one the first and second PBS of the fundamentalfilter cell and the first and second PBD of the harmonic filter cellsymmetrically split and combine the optical signals between the fastdelay path and the slow delay path of the corresponding filter celldepending on the optical signals' polarization.
 28. An opticalinterleaver as recited in claim 7, wherein the first and second PBS ofthe fundamental filter cell and the first and second PBS of the harmonicfilter cell each comprise at least one prism and a parallel plate.